Berezinskii-Kosterlitz-Thouless transition and anomalous metallic phase in a hybrid Josephson junction array

被引:0
|
作者
Bottcher, C. G. L. [1 ,5 ]
Nichele, F. [1 ,6 ]
Shabani, J. [2 ,7 ]
Palmstrom, C. J. [2 ,3 ,4 ]
Marcus, C. M. [1 ]
机构
[1] Univ Copenhagen, Niels Bohr Inst, Ctr Quantum Devices, DK-2100 Copenhagen, Denmark
[2] Univ Calif Santa Barbara, Calif Nanosyst Inst, Santa Barbara, CA 93106 USA
[3] Univ Calif Santa Barbara, Dept Elect Engn, Santa Barbara, CA 93106 USA
[4] Univ Calif Santa Barbara, Mat Dept, Santa Barbara, CA 93106 USA
[5] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
[6] IBM Res Lab, Zurich, Switzerland
[7] New York Univ, New York, NY 10003 USA
基金
新加坡国家研究基金会;
关键词
MAGNETIC-FIELD; QUANTUM; SUPERCONDUCTIVITY; STATE; ENHANCEMENT; BEHAVIOR; FILMS;
D O I
10.1103/PhysRevB.110.L180502
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We investigate the Berezinskii-Kosterlitz-Thouless (BKT) transition in a semiconductor-superconductor two-dimensional Josephson junction array. Tuned by an electrostatic top gate, the system exhibits separate superconducting (S), anomalous metal (M*), and insulating (I) phases, bordered by separatrices of the temperature-dependent sheet resistance Rs. We find that the gate-dependent BKT transition temperature falls to zero at the S-M* boundary, suggesting incomplete vortex-antivortex pairing in the M* phase. In the S phase, Rs is roughly proportional to the perpendicular magnetic field at the BKT transition, as expected, while in the M* phase, Rs deviates from its zero-field value as a power law in the field with exponent close to 1/2 at low temperature. An in-plane magnetic field eliminates the M* phase, leaving a small scaling exponent at the S-I boundary, which we interpret as a remnant of the incipient M* phase.
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页数:7
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